[0001] This invention relates to shadow mask type colour cathode ray tubes, and, more particularly,
to the shadow mask.
[0002] In general, a shadow mask type colour cathode ray tube comprises an electron gun
in the tube emitting three electron beams, a shadow mask distributing these beams
selectively by colour, and a phosphor screen emitting light in the three colours,
red, green and blue, on excitation by these beams. The image formed on the screen
is observed through an envelope panel. In the shadow mask there are provided a large
number of apertures which correspond precisely with the phosphor pattern of the respective
colour on the screen. As the effective electron beams passing through these apertures
during colour cathode ray tube operation represent somewhat less than a third of the
incoming beams, the rest of the electrons impinge on the shadow mask and their energy
is converted into heat energy, raising the temperature of the shadow mask. In a normal
operating television set, the shadow mask is thereby heated to a temperature of about
80 C. In the special colour cathode ray tubes used in the instrument panels in aircraft
cockpits, the shadow mask temperature can rise to around 200°C. Most shadow masks
consist of a lamina 0.1 to 0.3 mm thick, made by cold rolling, of which the main constituent
is iron of thermal expansion coefficient 1.2 x 10
-5/°C. The rigid L section mask frame that supports the shadow mask skirt is about 1mm
thick, is likewise made by cold rolling, and is subjected to blackening treatment.
Thermal expansion readily occurs when the shadow mask is heated. Since the shadow
mask periphery is adjacent to the blackened mask frame, which has a large heat capacity,
heat is transferred from the shadow mask periphery to this mask frame by radiation
or conduction. This results in the temperature of the shadow mask periphery falling
below the temperature at its center, producing a temperature difference between the
center and periphery. This produces the "doming" phenomenon caused by relative thermal
expansion taking place principally at the center. Consequently the distance between
the shadow mask and phosphor screen alters, disturbing the accurate landing of the
electron beams and thus impairing colour purity. This phenomenon of mislanding due
to doming is particularly evident when the colour cathode ray tube has just been switched
on. Also, if part of the picture is locally of high luminance and especially if such
high luminance portions are stationary for some time, high electron flow density regions
occur on the shadow mask, causing local doming.
[0003] With regard to this doming phenomenon in colour cathode ray tubes, there have been
a number of proposals aimed at promoting dispersal of heat from the center of the
shadow mask. For instance, in U.S. Patent No. 2826538 ( Hunter et al.), it is proposed
to facilitate shadow mask heat dispersal by providing a black layer of graphite on
the shadow mask surface. Such a graphite layer in the colour cathode ray tube acts
as an excellent radiator, lowering the shadow mask temperature. However, such a black
graphite layer has the following drawbacks. The thermal cycle of the heating process
involved in the manufacture of the colour cathode ray tube impairs the adhesion of
the black layer so that when the colour cathode ray tube is subjected to vibration,
part of this layer separates and minute flakes fall off. When this happens, flakes
adhering to the shadow mask cause blockage of the electron apertures, adversely affecting
the characteristics of the image on the phosphor screen. Flakes adhering to the electron
gun cause sparks between the electrodes, impairing the withstand voltage characteristic,
and so forth, so that the quality of the colour cathode ray tube is markedly reduced.
[0004] It has been proposed, in Japanese Patent Application No.58-148843 (Disclosure No.60-54139),
to control doming by using high temperature heat treatment to seal lead borate glass
to the surface of the shadow mask. However, since this glass layer, which is bonded
to the surface of the shadow mask, contains a great deal of lead (which has a very
high atomic number), it is difficult to reduce the elastic reflection of the electrons
impinging on the shadow mask. In Japanese Patent Publication No. 49-14777, a proposal
was made to prevent such electron scattering by nickel plating the vicinity of the
mask apertures. However, the method of manufacture is not practical because it is
too complicated, and electron scattering by the surface of the shadow mask apart from
the apertures cannot be altogether eliminated. Electron scattering causes emission
of light from undesired parts of the screen, spoiling image contrast, and lowering
colour purity.
[0005] It is an object of this invention to provide a colour cathode ray tube of improved
picture contrast and purity drift characteristics by decreasing elastic reflection
of the electron beams at the shadow mask surface and controlling expansion resulting
from shadow mask heat evolution produced by the electron beams.
[0006] According to this invention, in a colour cathode ray tube equipped with: a phosphor
screen; a shadow mask adjacent this screen and provided with a large number of through-holes
or apertures: and an electron gun arranged on the opposite side of the shadow mask
to said phosphor screen; wherein the electron beam emitted from the electron gun pass
through the through-holes of the shadow mask to impinge on the screen; in at least
a part of the shadow mask surface, a layer is formed that includes one substance selected
from the group consisting of: metal, metal oxide, metal carbide, metal nitride and
mixture thereof; using as a binder a substance selected from the group consisting
of: amorphous metal oxide, amorphous metal hydroxide and mixture thereof. This layer
on the shadow mask is obtained by applying, to the surface of the shadow mask provided
with a large number of holes, a suspension containing a metal alkoxide compound, then
subjecting the shadow mask to heat treatment.
[0007] Any desired alkoxide, such as a methoxide M(OCH
3)
n (where M means a metal), ethoxide M(OC
2H
5)
n, n-pro
poxide 2 M(O.n-C
3H
7)
n, or isopropoxide M(O.iso-C
3H
7)
n, buthoxide 3 7 3 7 M(O.n-C
4H
9)
n, or isobuthoxide M(O.iso-C
4H
9)
n may be used. Those which are readily soluble at ordinary temperature in water-soluble
low alcohols such as methanol, ethanol, or propanol are easiest to handle industrially.
[0008] According to this invention, the rise in temperature of the shadow mask is limited
since the thermal radiation coefficient of this layer is high, so heat can easily
escape. Since the volume resistivity of the layer is large, when a large current flows,
the layer absorbs electrons and acquires a negative charge, which applies an electrostatic
correction to the beam. Furthermore, electron scattering is reduced because the atomic
number of the metal contained in the layer is low. Additionally this layer increases
the residual emission either by gas adsorption or by suppressing gas generation, since
it is finely formed on the shadow mask.
[0009] In order that the invention may be more readily understood, it will now be described,
by way of example only, with reference to the accompanying drawings, in which:-
Fig. 1 is an axial cross-sectional view of an embodiment of this invention.
Fig. 2 is an enlarged perspective view showing part of the shadow mask of this embodiment
in Fig. 1.
Fig. 3 and Fig. 4 are schematic illustrations of the reproduced picture pattern, given
in explanation of the purity drift characteristics of this embodiment of the invention.
Fig. 5 is a schematic illustration of the reproduced picture pattern, given in explanation
of the contrast characteristics of this embodiment of the invention.
Fig. 6 is a partial cross-sectional view showing another embodiment of this invention.
Fig. 7 is a characteristic graph showing the relationship between layer thickness
and amount of beam movement for a product used for comparison, for the case of the
pattern shown in Fig. 4.
[0010] As shown in Fig. 1, the shadow mask type colour cathode ray tube of this embodiment
is provided with an evacuated envelope consisting of an essentially rectangular panel
1, a funnel 2 and a neck 3. The inside of panel 1 is coated with a phosphor screen
4 formed by a phosphor layer in the form of stripes that emit respectively red, green
and blue light. In-line electron guns 6 that emit three electron beams corresponding
to red, green and blue are arranged in neck 3 in'line along the horizontal axis of
panel 1. A shadow mask 7, wherein a large number of slot-shaped apertures are arranged
in the vertical direction and a large number of vertical rows thereby are provided
in the horizontal direction, is fixedly supported by a mask frame 8 at a position
adjacent to and opposite phosphor screen 4. Mask frame 8 is supported within the panel
by means of stud pins 10 embedded in the inside wall of the vertical edge of panel
1 by means of resilient members 9.
[0011] The three in-line electron beams 5 are deflected by a deflecting device 12 provided
outside funnel 2 so that they are scanned over a rectangular area corresponding to
rectangular panel 1. The colour picture is reproduced by colour-selecting these beams
landing on the phosphor stripe layer through the apertures of shadow mask 7. In some
cases, the electron beams may,not land accurately on the phosphor stripes for which
they are intended, due to the effect of external magnetic fields such as the earth's
magnetic field. This spoils the colour purity of the picture. To prevent this, a magnetic
shield 11 of high permeability, made of high permeability metal sheet, is fastened
to the inside of the funnel 2 by means of frame 8.
[0012] The material of the shadow mask is for example low carbon steel sheet of thickness
0.1mm to 0.3mm whose main constituent is iron. A photo-resist film is obtained on
both sides of this shadow mask by applying and then drying a photo-sensitive liquid
consisting of for example alkali milk caseinate and ammonium bichromate. Next, a negative
mask provided with the prescribed hole pattern is tightly stuck onto this photo-resist
film and developed by exposure, so as to expose those parts of the metal surface where
the through-holes are to be formed. Then through-holes having the prescribed aperture
shape are formed by spraying etching liquid comprising ferric chloride onto the exposed
metal surface. This shadow mask blank, in the form of a flat sheet formed with through-holes,
is mounted in a prescribed outer frame. Its edges are clamped by a blank holder and
die, and its main area, that is provided with the through-holes, is formed to the
prescribed curved surface by a punch above and a knockout below. Its peripheral region
is then bent over for example in the axial direction to provide a skirt for supporting
and holding the main area of the mask. The skirt of the thus-formed shadow mask is
supported and fixed in a rigid frame of for example L-shaped cross- section.
[0013] Next, a film of thickness about 15 micron is applied to one side of the main area
of the shadow mask, where the through-holes are provided, by spraying a suspension
of for example, as in the following Example, an alkoxide of silicon and zirconia,
e.g. Si(OC
2H
5) + Zr(OC
4H
9)
4, containing 494 silicon zirconate (ZrSi0
4) as a filler, onto the main area of the mask, which is concave towards the electron
gun when it is arranged adjacent the screen. The filler is desired to be of a material
containing metal component with smaller atomic number than that of lead.
Example
[0014]

[0015] Various methods may be used to apply this suspension. The requirements which such
methods must satisfy are that the suspension must be applied uniformly and the through-holes
must not get blocked. Painting the suspension on using a brush, for example, is undesirable
due to the risk of producing a non-uniform coating and blocking'the holes. In this
respect, with the spraying method, if the suspension is applied with a spraying pressure
of about 3kg/cm
2 from a distance of 20cm to 30cm, a film of thickness about 15 micron as in the above
Example can be formed in about 10 seconds. This is the preferred method for mass production
since if there should be any foreign bodies stuck in the through-holes, they will
be removed by the high pressure suspension liquid hitting the.back of the mask.
[0016] Thus a layer 13 as shown in Fig. 2 can be obtained by heating, in an atmosphere at
70°C or above, a shadow mask coated, on the surface facing the electron guns, with
a suspension of an alkoxide compound of silicon and zirconia, containing zircon as
a filler. The alkoxide compound of silicon and zirconia applied to shadow mask 7 undergoes
hydrolysis due to the moisture in the air etc. in an atmosphere at 70
0C or over, resulting in the formation of a film by a polycondensation reaction between
the alkoxides, forming a zircon-containing mixed layer of amorphous silicon and zirconia
metal oxides and metal hydroxides. Although in the above example, the suspension was
heated after application, to shorten the manufacturing time, if the suspension is
applied while heating to 70
0C or more, the subsequent heat treatment step can be dispensed with. Also, since the
alkoxide compound of silicon and zirconia has a good radiation absorption characteristic
in the infra-red region, it has been found that satisfactory film formation can be
achieved even at ordinary temperatures, without using an atmosphere of over 70 C,
by irradiating the surface of the shadow mask with for example infra-red radiation
whilst the suspension containing the alkoxide compound of silicon and zirconia is
being applied. It is also possible to irradiate with infra-red radiation after applying
the suspension.
[0017] Once thus-completed shadow mask 7 has been assembled with the panel, the screen forming
step is carried out. First of all, an azide photo-resist film is formed on the inside
face of the panel, and exposed through through-holes 7a of shadow mask 7 using an
ultra-high pressure mercury lamp. After developing the resist film, the graphite is
applied and dried, developed using a decomposing agent, and narrow light-absorbing
strips formed at prescribed positions on the inside face of the panel. Next, phosphor
particles, in the form for example of a slurry to which phosphor particles for blue
have been added, are applied on the inside face of the panel, onto a photoresist film
consisting of ammonium dichromate and polyvinyl alcohol. Exposure and developing are
then performed as above to form blue- emitting phosphor strips. Green-emitting and
red-emitting phosphor strips are then successively formed in the same way to obtain
the screen.
[0018] When the panel has been completed by the above steps, it is bonded to the funnel
using frit glass and, after exhausting and sealing, the prescribed steps are performed
to obtain the colour cathode ray tube.
[0019] The purity drift characteristics obtained by the inventors for 21 inch colour cathode
ray tubes manufactured as above were as follows. The sample screen picture patterns
used for these experiments are shown in Fig. 3 and Fig. 4. The pattern of Fig. 3 is
one in which the whole screen is white, while the pattern of Fig. 4 is one in which
part of the screen is white. In the Fig. 4 pattern, there are two white bands 51 of
horizontal width 75mm disposed on the left and right respectively with their centers
140mm from the center of the screen, the rest of the screen being black i.e. not emitting
light. The symbol x indicates the measurement points. The results of measurement of
the amount by which the beams are displaced are shown in Table 1. The measurement
conditions were Eb = 26.5 kV. Ik in the case of pattern (A) is 1,500 microamp, and
in the case of pattern (B) is 1,100 microamp.

[0020] The comparative examples in the above Table were provided by 21 inch colour cathode
ray tubes wherein, by heating at high temperature, lead borate glass was sealed and
bonded in about 20 micron thickness to the surface, facing the electron guns, of shadow
masks constructed as proposed in Japanese Patent Application No. 58-148843 (Patent
Disclosure No.60-54139) invented by the present inventor and others. The inventors
found that the purity characteristic of colour cathode ray tubes according to this
invention was better than that of the prior art colour cathode ray tubes. This was
because the thermal emissivity (about 0.9) of the zircon-containing layer formed on
the shadow mask is much greater than that of the prior art shadow mask, so radiation
of heat from the shadow mask is promoted thereby limiting the rise in temperature
of the shadow mask. Fig. 7 shows the improvement of the beam displacement characteristic,
in comparison with the prior art, for the pattern of Fig. 4, obtained by varying the
thickness of the applied layer. As can be seen from this graph, the preferred range
of thickness is 1 micron to 30 micron. In this embodiment, zircon was used as the
filler. However, the essence of this invention is not restricted to this, and a similar
improvement in thermal emissivity and purity drift characteristic can be obtained
by using dark pigments comprising other metal oxides, such as cobalt oxide, chromium
oxide, iron oxide, or manganese oxide. Also carbides, such as silicon carbide, boron
carbide, tungsten carbide etc. can be used as fillers with the same effect. No doubt
this is because the thermal conductivity of these carbides is greater than that of
the mild steel sheet, facilitating removal of heat generated in the shadow mask. Specifically,
the thermal conductivity of the mild steel sheet is 0.11 cal/cm.sec C, while that
of silicon carbide is 1.0 cal/cm.sec
oC, that of boron carbide is 0.65 cal/cm.sec C, and that of tungsten carbide is 0.7
cal/cm.sec oC. Also nitrides, such as silicon nitride, boron nitride, or aluminium
nitride etc. can be used as fillers with the same effect. It is believed this is because
the volume resistivity of these nitrides is large (10
12 ohm-
m to 10
14 ohm-m), so that when a large current flows, this layer acts as an electron-absorbing
layer, becoming negatively charged. As a result, it is able to exert an electrostatic
correction effect on the electron beams, which improves the purity drift characteristic.
A similar effect is obtained by use of tungsten, lead, or bismuth etc.
[0021] In the above embodiment the use of a compound of silicon and zirconia for the metal
alkoxide compound is described. However, as in the case of the filler, the essence
of the invention is not restricted to this, and alkoxide compounds of for example
silicon, silicon and titanium, silicon and aluminium, titanium and zirconium etc.
can be used.
[0022] Next, for purposes of comparison, the contrast characteristic of a colour cathode
ray tube manufactured with a shadow mask according to Japanese Patent Application
No. 58-148843 referred to above but otherwise similarly to the colour cathode ray
tube of this invention described above was obtained. For the purposes of the test,
the picture pattern shown in Fig. 5 was reproduced. A white portion 31 of dimensions
300mm x 100mm was disposed in the middle of the top of this screen 30, the remainder
32 being black. The measurement points, referred to as rfl and rf2, are indicated
by the symbol x and are located respectively 30mm and 60mm below the center of the
screen. The luminance at these points rfl and rf2 is shown in Table 2. The measurement
conditions were that the anode voltage Eb of the colour cathode ray tube was 26.5
kV, the total cathode current Ik was 500 micro-amp, and the colour of the white colour
was 9,300°K + 27MPCD.

[0023] It can be seen from Table 2 that the luminance of the dark portion is reduced in
this embodiment of the invention. This means that the.elastic scattering of electrons
is decreased. This is dependent on the atomic numbers of the Si and Zr constituents
of coating layer 13 (their atomic numbers are 14 and 40 respectively) being lower
than the atomic numbers 82 and 56 of the Pb and Ba of the lead borate glass of the
comparison product.
[0024] The residual emission percentage after subjecting a colour cathode ray tube according
to this embodiment to a 3,000 hours continuous operation test was then determined.
It was found that the residual emission percentage was indeed improved, being 80%
of the initial value. For the prior art product, a residual emission percentage of
70% is standard. Thus this represents an improvement of better than 10%. This is inferred
to be because of gas adsorption by the coating layer of this embodiment. The amorphous
silicon oxide (Si0
2) that is used as a binder appears to be particularly effective in this respect.
[0025] Also it is thought that generation of gas is suppressed by the formation of a fine
coating layer on the shadow mask surface. It is therefore particularly effective to
form the coating on the surface of the shadow mask facing the electron guns, since
this surface reaches a very high temperature when the electron beams impinge on it
and so tends to generate unstable gases. Of course, formation of such a coating increases
the manufacturing process, but, as shown in Fig. 6, if the whole of the shadow mask
surface is covered by coating 13 according to this invention, practically all generation
of unstable gases by the shadow mask can of course be suppressed.
[0026] In the description of this embodiment, the suspension containing an alkoxide compound
of zircon and silicon and zirconia was applied to the shadow mask before forming the
phosphor screen, and a mixed zircon-containing layer of silicon and zirconia amorphous
metal oxides and metal hydroxides was formed. However, if the presence of this coating
layer causes a slight adverse photochemical effect in the exposure step when forming
the phosphor screen, the formation of this coating can be carried out after formation
of the phosphor screen.
[0027] If the coating of this invention is formed on the surface of the shadow mask facing
electron guns, it is not necessary to form a conductive coating. By this means, a
5 to 10% improvement in the purity drift characteristic can be obtained compared with
the case where a conductive coating is formed.
[0028] As described above, according to this invention, a colour cathode ray tube can be
obtained with improved contrast and purity drift characteristics, a better emission
life characteristic, and which is well adapted for mass production.
1. A colour cathode ray tube comprising:
a phosphor screen (4);
a shadow mask (7) with a large number of apertures, arranged in the vicinity of said
phosphor screen;
an electron gun (6) generating an electron beam (5) passing through said apertures
of said shadow mask to excite said phosphor screen;
characterized in that said shadow mask (7) is coated with a layer (13) consisting
essentially of a binder selected from the group consisting of amorphous metal oxide,
amorphous metal hydroxide and mixture thereof; and
a filler selected from the group consisting of metal, metal oxide, metal carbide,
metal nitride and mixture thereof.
2. The colour cathode ray tube according to claim 1 wherein said layer is formed on
a surface of said shadow mask facing said electron gun.
3. The colour cathode ray tube according to claim 1 wherein said binder is a product
of heat treatment of a metal alkoxide compound.
4. The colour cathode ray tube according to claim 3 wherein metal of said metal alkoxide
compound is one selected from the group consisting of silicon, titanium, aluminium,
zirconium and mixsture thereof.
5. The colour cathode ray tube according to claim 1 wherein said filler is one selected
from the group consisting of silicon carbide, manganese oxide, chromium oxide, iron
oxide, cobalt oxide, copper oxide, zircon, zirconium and mixture thereof.
6. The colour cathode ray tube according to claim 1 wherein the thickness of said
layer is 1 micron to 30 micron.
7. The colour cathode ray tube according to claim 1 wherein the filler is dark in
colour.